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In many problems involving application of Newton's Second Law to the motion of solid objects, friction is neglected for the sake of making the solution easier. The counterpart of friction between solids is viscosity of liquids. Do problems involving fluid flow become simpler if viscosity is neglected? Explain.

Short Answer

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Short Answer: Neglecting viscosity in fluid flow problems may simplify certain cases, such as the flow of an ideal fluid or the inviscid flow approximation. However, it is not always an ideal approach, as viscosity often plays an essential role in real-world applications. Ignoring viscosity can lead to inaccurate predictions and limited understanding of the physical behavior of the fluid. Therefore, the complexity of fluid flow problems depends on the specific problem, and the choice to neglect viscosity should be carefully considered based on the problem's context and desired accuracy.

Step by step solution

01

Role of Viscosity in Fluid Mechanics

Viscosity is the measure of a fluid's resistance to flow. It is a property of the fluid that causes internal resistance to motion between its particles. Viscosity plays a significant role in fluid mechanics, as it determines how fluid particles interact with each other and with solid surfaces. In fluid flow problems, the presence of viscosity often leads to complicated mathematical models as the velocity gradients in the fluid must be taken into consideration.
02

Examples of Simple Fluid Flow Problems

There are cases where problems involving fluid flow can be simplified by neglecting viscosity. One example is the flow of an ideal fluid or a perfect fluid, which assumes that the fluid has zero viscosity. In this case, the fluid particles are assumed to not experience any internal resistance, and the fluid flow is described by the Euler equation, which is generally easier to solve than the full set of fluid equations involving viscosity. Another example is the inviscid flow approximation, which neglects the viscous effects in the fluid flow, assuming that they are small compared to other forces acting on the fluid particles.
03

Complexity of Neglecting Viscosity

Neglecting viscosity may make some fluid flow problems easier to solve, but it is not always an ideal approach. In real-world applications, viscosity is often an important factor in fluid flow problems as it influences the rate of heat transfer, energy loss, and stress on solid boundaries. Neglecting viscosity can lead to inaccurate predictions and a lack of understanding of the physical behavior of the fluid. In conclusion, while neglecting viscosity may simplify certain fluid flow problems, it is not always a recommended approach since it can lead to unrealistic solutions and an incorrect understanding of fluid behavior. The complexity of fluid flow problems depends on the specific problem at hand, and the choice of neglecting viscosity should be carefully considered based on the problem's context and the desired level of accuracy.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Newton's Second Law
Understanding the dynamics of fluid mechanics starts with one of the fundamental principles of physics: Newton's Second Law. This law states that the force acting on a body is equal to the mass of the body multiplied by its acceleration (\( F = ma \)). When applied to fluid mechanics, this principle helps in analyzing the forces acting on fluid particles as they move and interact. This is crucial, especially in determining how changes in velocity lead to differences in pressure and flow patterns within the fluid.

In fluid dynamics, the application of Newton's Second Law often involves complex calculations, as the motion of fluid particles can be influenced by numerous factors, including viscosity, which adds an internal resistance to space and complicates the relationship between force, mass, and acceleration.
Resistance to Flow
Resistance to flow in fluid mechanics is largely attributed to a property known as viscosity. Viscosity describes how thick or sticky a fluid is, which translates to the ease or difficulty with which the fluid particles move past each other. Imagine honey and water; honey has a higher viscosity and thus, a greater resistance to flow. When considering fluid flow problems, higher resistance due to viscosity leads to more complex calculations, as it requires accounting for the shear stress and the velocity gradient within the fluid. This internal friction can influence everything from the fluid's velocity profile to the energy required to pump it through a pipe system.
Euler Equation
The Euler equation is a simplified form of the Navier-Stokes equations, which are the fundamental equations for fluid flow. It is derived under the assumption of an inviscid (zero viscosity) fluid, implementing the principle of conservation of momentum. The Euler equation describes how pressure, velocity, and density interact in the flow of an ideal fluid.

In reality, absolutely inviscid fluids don't exist, but the Euler equation provides a valuable approximation for situations where the effects of viscosity are minimal and can be reasonably neglected, such as in high-speed aerodynamics or in the bulk flow away from solid boundaries.
Inviscid Flow Approximation
The inviscid flow approximation is a simplifying assumption in fluid mechanics where the fluid's viscosity is assumed to be negligible. This approximation allows for the analysis of fluid flows without having to consider viscous forces, making the governing equations much simpler to solve. It is used in scenarios where the effects of viscosity on the overall flow are small, such as in flow around airplane wings at high altitudes or in pipelines with very turbulent flow. Although this assumption can yield solutions that are easier to compute, it may not capture important features of the flow near solid surfaces where viscous forces are significant.
Fluid Flow Problems
Fluid flow problems can present a wide array of challenges, depending on the complexities involved within the flow field. These complexities often come from factors like changes in fluid speed, variations in cross-sectional area of the flow, interactions with solid boundaries, and the presence of viscosity. While inviscid flow models simplify these problems, real-world applications require more precision, and therefore, a more detailed approach that considers viscous effects. Engineers and physicists use different mathematical models and computational fluid dynamics (CFD) to predict the behavior of fluid flows accurately for tasks such as designing efficient hydraulic systems, improving aerodynamic performance, or predicting weather patterns.

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Most popular questions from this chapter

Brass weights are used to weigh an aluminum object on an analytical balance. The weighing is done one time in dry air and another time in humid air. What should the mass of the object be to produce a noticeable difference in the balance readings, provided the balance's sensitivity is \(m_{0}=0.100 \mathrm{mg} ?\) (The density of aluminum is \(\rho_{\mathrm{A}}=2.70 \cdot 10^{3} \mathrm{~kg} / \mathrm{m}^{3}\); the density of brass is \(\rho_{11}=8.50 \cdot 10^{3} \mathrm{~kg} / \mathrm{m}^{3}\), The density of the dry air is \(1.2285 \mathrm{~kg} / \mathrm{m}^{3}\), and the density of the humid air is \(1.2273 \mathrm{~kg} / \mathrm{m}^{3}\).).

An airplane is moving through the air at a velocity \(v=200, \mathrm{~m} / \mathrm{s}\) Streamlines just over the top of the wing are compressed to \(80.0 \%\) of their original cross-sectional area, and those under the wing are not compressed at all. a) Determine the velocity of the air just over the wing. b) Find the difference in the pressure of the air just over the wing, \(P\), and that of the air under the wing, \(P\). The density of the air is \(1.30 \mathrm{~kg} / \mathrm{m}^{3}\). c) Find the net upward force on both wings due to the pressure difference, if the area of the wings is \(40.0 \mathrm{~m}^{2}\).

Many altimeters determine altitude changes by measuring changes in the air pressure. An altimeter that is designed to be able to detect altitude changes of \(100 \mathrm{~m}\) near sea level should be able to detect pressure changes of a) approximately I Pa. d) approximately \(1 \mathrm{kPa}\). b) approximately 10 Pa. e) approximately \(10 \mathrm{kPa}\). c) approximately \(100 \mathrm{~Pa}\).

Calculate the ratio of the lifting powers of helium (He) gas and hydrogen \(\left(\mathrm{H}_{2}\right)\) gas under identical circumstances. Assume that the molar mass of air is \(28.95 \mathrm{~g} / \mathrm{mol}\).

Water at room temperature flows with a constant speed of \(8.00 \mathrm{~m} / \mathrm{s}\) through a nozzle with a square cross section, as shown in the figure. Water enters the nozzle at point \(A\) and exits the nozzle at point B. The lengths of the sides of the square cross section at \(A\) and \(B\) are \(50.0 \mathrm{~cm}\) and \(20.0 \mathrm{~cm}\), respectively. a) What is the volume flow rate at the exit? b) What is the acceleration at the exit? The length of the nozzle is \(2.00 \mathrm{~m}\). c) If the volume flow rate through the nozzle is increased to \(6.00 \mathrm{~m}^{3} / \mathrm{s}\). what is the acceleration of the fluid at the exit?

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